{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:AVWVG7KGY6BM3DNAURWJ6VVJ7I","short_pith_number":"pith:AVWVG7KG","schema_version":"1.0","canonical_sha256":"056d537d46c782cd8da0a46c9f56a9fa082e5ef42251c966473d68f14ce2f7ef","source":{"kind":"arxiv","id":"2405.17341","version":3},"attestation_state":"computed","paper":{"title":"Searching for signatures of new physics in $B \\to K \\, \\nu \\, \\overline{\\nu}$ to distinguish between Dirac and Majorana neutrinos","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C. S. Kim, Dibyakrupa Sahoo, K. N. Vishnudath","submitted_at":"2024-05-27T16:47:50Z","abstract_excerpt":"We conduct a model-independent analysis of the distinct signatures of various generic new physics possibilities in the decay $B \\to K \\, \\nu \\, \\overline{\\nu}$ by analyzing the branching ratio as well as the missing mass-square distribution. Considering the final neutrinos to be of the same flavor with non-zero mass, we discuss the new physics contributions for both Dirac and Majorana neutrino possibilities. In our study, we utilize the analytical relations among form factors in semi-leptonic $B \\to K$ transitions, which are consistent with current lattice QCD predictions to a very high numeri"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2405.17341","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-05-27T16:47:50Z","cross_cats_sorted":[],"title_canon_sha256":"ae32fccdbebe476e84d33924af986ae2a33e70ac154ee2e6cebe92b3ab62032c","abstract_canon_sha256":"0b5ddd628be5f58cd839763d6d167176c1fd1076b4ee452479367ada51d150a6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:02:20.265722Z","signature_b64":"1f18dxI5IpVWu5xVbDVGqtxeITC1cTKRq4HT0jR9i2jjP7bEYwRmgslZBibdyeOfWcjkpHs4s0fp8pnByPu3Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"056d537d46c782cd8da0a46c9f56a9fa082e5ef42251c966473d68f14ce2f7ef","last_reissued_at":"2026-07-05T09:02:20.265243Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:02:20.265243Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Searching for signatures of new physics in $B \\to K \\, \\nu \\, \\overline{\\nu}$ to distinguish between Dirac and Majorana neutrinos","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C. S. Kim, Dibyakrupa Sahoo, K. N. Vishnudath","submitted_at":"2024-05-27T16:47:50Z","abstract_excerpt":"We conduct a model-independent analysis of the distinct signatures of various generic new physics possibilities in the decay $B \\to K \\, \\nu \\, \\overline{\\nu}$ by analyzing the branching ratio as well as the missing mass-square distribution. Considering the final neutrinos to be of the same flavor with non-zero mass, we discuss the new physics contributions for both Dirac and Majorana neutrino possibilities. In our study, we utilize the analytical relations among form factors in semi-leptonic $B \\to K$ transitions, which are consistent with current lattice QCD predictions to a very high numeri"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.17341","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2405.17341/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2405.17341","created_at":"2026-07-05T09:02:20.265305+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.17341v3","created_at":"2026-07-05T09:02:20.265305+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.17341","created_at":"2026-07-05T09:02:20.265305+00:00"},{"alias_kind":"pith_short_12","alias_value":"AVWVG7KGY6BM","created_at":"2026-07-05T09:02:20.265305+00:00"},{"alias_kind":"pith_short_16","alias_value":"AVWVG7KGY6BM3DNA","created_at":"2026-07-05T09:02:20.265305+00:00"},{"alias_kind":"pith_short_8","alias_value":"AVWVG7KG","created_at":"2026-07-05T09:02:20.265305+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2507.10801","citing_title":"Probing vector- vs scalar-mediator dark-matter scenarios in $B\\to (K,K^*) M_X$ decays","ref_index":20,"is_internal_anchor":false},{"citing_arxiv_id":"2601.08907","citing_title":"Dark Matter emission at Belle II and NA62 in Minimal Flavor Violation framework","ref_index":11,"is_internal_anchor":false},{"citing_arxiv_id":"2604.20340","citing_title":"Baryon-Meson Sum Rule for $b \\to s \\nu\\bar\\nu$","ref_index":55,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/AVWVG7KGY6BM3DNAURWJ6VVJ7I","json":"https://pith.science/pith/AVWVG7KGY6BM3DNAURWJ6VVJ7I.json","graph_json":"https://pith.science/api/pith-number/AVWVG7KGY6BM3DNAURWJ6VVJ7I/graph.json","events_json":"https://pith.science/api/pith-number/AVWVG7KGY6BM3DNAURWJ6VVJ7I/events.json","paper":"https://pith.science/paper/AVWVG7KG"},"agent_actions":{"view_html":"https://pith.science/pith/AVWVG7KGY6BM3DNAURWJ6VVJ7I","download_json":"https://pith.science/pith/AVWVG7KGY6BM3DNAURWJ6VVJ7I.json","view_paper":"https://pith.science/paper/AVWVG7KG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.17341&json=true","fetch_graph":"https://pith.science/api/pith-number/AVWVG7KGY6BM3DNAURWJ6VVJ7I/graph.json","fetch_events":"https://pith.science/api/pith-number/AVWVG7KGY6BM3DNAURWJ6VVJ7I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AVWVG7KGY6BM3DNAURWJ6VVJ7I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AVWVG7KGY6BM3DNAURWJ6VVJ7I/action/storage_attestation","attest_author":"https://pith.science/pith/AVWVG7KGY6BM3DNAURWJ6VVJ7I/action/author_attestation","sign_citation":"https://pith.science/pith/AVWVG7KGY6BM3DNAURWJ6VVJ7I/action/citation_signature","submit_replication":"https://pith.science/pith/AVWVG7KGY6BM3DNAURWJ6VVJ7I/action/replication_record"}},"created_at":"2026-07-05T09:02:20.265305+00:00","updated_at":"2026-07-05T09:02:20.265305+00:00"}